(a) For the radiation of frequency (greater than threshold frequency of metal )photoelectric current is directly proportional to the intensity of incident radiation. So the increase in intensity of incident radiation increases the photoelectric current.
(b) As, `eV_0=hv-phi_0 or V_0=(hv)/e-(phi_0)/e......(i)` so stopping potential `V_0` is directly proportional to frequency v. So the graph (i) is a st. line equation. Comparing it a straight line equation y=mx+C, we have slope of his line =h/e =a constant. So slope of `V_0` and v graph =h/e which is constant for all surfaces.
(c) Max `KE=eV_0=hv-phi_0`. It is independent of intensity of incident radiation till v is constant.